A diffusive Fisher-KPP equation with free boundaries and time-periodic advections

preprint2016arXivOpen access

Abstract

We consider a reaction-diffusion-advection equation of the form: ut=uxx−β(t)ux+f(t,u)u_t=u_{xx}-β(t)u_x+f(t,u) for x∈(g(t),h(t))x\in (g(t),h(t)), where β(t)β(t) is a TT-periodic function representing the intensity of the advection, f(t,u)f(t,u) is a Fisher-KPP type of nonlinearity, TT-periodic in tt, g(t)g(t) and h(t)h(t) are two free boundaries satisfying Stefan conditions. This equation can be used to describe the population dynamics in time-periodic environment with advection. Its homogeneous version (that is, both ββ and ff are independent of tt) was recently studied by Gu, Lou and Zhou \cite{GLZ}. In this paper we consider the time-periodic case and study the long time behavior of the solutions. We show that a vanishing-spreading dichotomy result holds when ββ is small; a vanishing-transition-virtual spreading trichotomy result holds when ββ is a medium-sized function; all solutions vanish when ββ is large. Here the partition of β(t)β(t) is much more complicated than the case when ββ is a real number, since it depends not only on the "size" βˉ:=1T∫0Tβ(t)dt\barβ:= \frac{1}{T}\int_0^T β(t) dt of β(t)β(t) but also on its "shape" β~(t):=β(t)−βˉ\tildeβ(t) := β(t) - \barβ.

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